Semiconductor element and semiconductor memory device using the same

ABSTRACT

A field-effect semiconductor element implemented with a fewer number of elements and a reduced area and capable of storing data by itself without need for cooling at a cryogenic temperature, and a memory device employing the same. Gate-channel capacitance is set so small that whether or not a trap captures one electron or hole can definitely and distinctively be detected in terms of changes of a current of the semiconductor FET element. By detecting a change in a threshold voltage of the semiconductor element brought about by trapping of electron or hole in the trap, data storage can be realized at a room temperature.

CROSS-REFERENCE TO RELATED APPLICATIONS

[0001] This application is a continuation application of Ser. No.08/778,260 filed on Jan. 8, 1997; which is a continuation application ofSer. No. 08/291,752 filed on Aug. 16, 1994, the entire disclosures ofwhich are hereby incorporated by reference.

BACKGROUND OF THE INVENTION

[0002] The present invention relates to a semiconductor element suitedfor integration with a high density and a semiconductor memory deviceimplemented by using the same.

[0003] Heretofore, polycrystalline silicon transistors have been used aselements for constituting a static random access memory device (referredto as SRAM in abbreviation). One of the relevant prior art techniques isdescribed in T. Yamanaka et al: IEEE International Electron DeviceMeeting, pp. 477-480 (1990). By making the most of polycrystallinesilicon transistors, integration density of the integrated circuit canbe enhanced, the reason for which can be explained by the fact that thepolycrystalline silicon transistor can be formed in stack or laminationatop a conventional bulk MOSFET (Metal-Oxide Semiconductor Field EffectTransistor) formed on a surface of a semiconductor substrate with aninsulation film being interposed between the polycrystalline silicontransistor and the bulk MOSFET. In the SRAM, implementation of a memorycell for one bit requires four bulk MOSFETs and two polycrystallinesilicon transistors. However, because the polycrystalline silicontransistors can be stacked atop the bulk MOSFETs, a single memory cellof the SRAM can be implemented with an area which substantiallycorresponds to that required for the bulk MOSFETs.

[0004] As another preceding technique related to the invention, theremay be mentioned a single-electron memory described in K. Nakazato etal: Electronics Letters, Vol. 29, No. 4, pp. 384-385 (1993). It isreported that a memory could have been realized by controlling electronon a one-by-one basis. It is however noted that the operationtemperature is as very low as on the order of 30 mK.

[0005] As a further prior art technique related to the invention, theremay be mentioned one which is directed to the study of RTN (RandomTelegraph Noise) of MOSFET, as is disclosed in F. Fang et al: 1990Symposium on VLSI Technology, pp. 37-38 (1990). More specifically, whena drain current of a MOSFET is measured for a predetermined time underthe constant-voltage condition, there makes appearance such phenomenonthat state transition takes place at random between a high-current stateand a low-current state. This phenomenon is referred to as the RTN, acause for which can be explained by the capture or entrapping of asingle electron in a level node existing at an interface between silicon(Si) and silicon oxide (SiO₂) and the release therefrom, whereby thedrain current undergoes variations. However, the RTN remains only as asubject for a fundamental study concerning the current noise in theMOSFET, and any attempt or approach for positively making use of the RTNin practical applications has not been reported yet at all.

[0006] At present, the technology for processing a semiconductorintegrated circuit with high fineness has developed up to such a levelwhere any attempt for realization of higher fineness will encounterdifficulty. Even if it is possible technologically, there will thenarise a problem that intolerably high cost is involved due to thenecessity for much sophisticated technique. Under the circumstances, agreat demand exists for a fundamentally novel method of enhancing theintegration density in the fabrication of semiconductor integratedcircuits instead of relying on a method of implementing thesemiconductor elements constituting the semiconductor integrated circuitsimply by increasing the fineness thereof.

[0007] On the other hand, the polycrystalline silicon transistor knownheretofore is basically equivalent to a variable resistor element in therespect that resistance between a source and a drain of thepolycrystalline silicon transistor can be controlled by a gate voltage.Consequently, implementation of a memory cell of a SRAM requires as manyas six semiconductor elements inclusive of the conventional MOSFETsformed in a silicon substrate.

[0008] By contrast, in the case of a DRAM (Dynamic Random AccessMemory), information or data of one bit can be stored in a memory cellconstituted by one MOSFET and one capacitor For this reason, the DRAMenjoys reputation as a RAM device susceptible to implementation with thehighest integration density. However, because the DRAM is based on sucha scheme that electric charge is read out onto a data wire of whichcapacitance is non-negligible, the memory cell thereof is required tohave capacitance on the order of several ten fF (femto-Farads), whichthus provides a great obstacle to an attempt for further increasingfineness in implementation of the memory cells.

[0009] By the way, it is also known that a nonvolatile memory devicesuch as a flash EEPROM (Electrically Erasable and Programmable Read-OnlyMemory) can be realized by employing MOSFETs each having a floating gateand a control gate. Further, as a semiconductor element for such anonvolatile memory device, there is known MNOS (Metal Nitride OxideSemiconductor) element. The MOOS is designed to store charge atinterface between a SiO₂-film and a Si₃N₄-film instead of the floatinggate of the flash EEPROM. Although the use of the MOSFET equipped withthe floating gate or the MNOS element is certainly advantageous in thatone-bit data can be held or stored by one transistor over an extendedtime span, a lot of time is required for the rewriting operation becausea current to this end has to flow through the insulation film, wherebythe number of times the rewriting operation can be performed is limitedto about 100 millions, which in turn gives rise to a problem thatlimitation is imposed to the applications which the nonvolatile memorydevice can find.

[0010] On the other hand, the one-electron memory device discussed inthe Nakazato et al's article mentioned hereinbefore can operate only ata temperature of cryogenic level, presenting thus a problem which isvery difficult to cope with in practice. Besides, a cell of thesingle-electron memory is comprised of one capacitor and two activeelements, which means that a number of the elements as required exceedsthat of the conventional DRAM, to a further disadvantage.

[0011] As will be appreciated from the forgoing, there exists a greatdemand for a semiconductor element which requires no capacitanceelements, differing from that for the DRAM and which can exhibit storedfunction by itself in order to implement a memory of higher integrationdensity than the conventional one without resorting to the technique forimplementing the memory with higher fineness.

SUMMARY OF THE INVENTION

[0012] In the light of the state of the art described above, it is anobject of the present invention to provide an epoch-making semiconductorelement which allows a semiconductor memory device to be implementedwith a lesser number of semiconductor elements and a smaller area andwhich per se has data or information storing capability while requiringno cooling at a low temperature such as cryogenic level.

[0013] Another object of the present invention is to provide asemiconductor memory device which can be implemented by using thesemiconductor elements mentioned above.

[0014] A further object of the invention is to provide a data processingapparatus which includes as a storage the semiconductor memory devicementioned above.

[0015] For achieving the above and other objects which will becomeapparent as description proceeds, it is taught according to a basictechnical concept underlying the invention that capacitance between agate and a channel of a semiconductor field-effect transistor element isset so small that capture of a single carrier (electron or hole) by atrap level can definitely and discriminately detected as a change in thecurrent of the semiconductor field-effect transistor element. Morespecifically, correspondences are established between changes in athreshold value of the semiconductor field-effect transistor element asbrought about by capture of a carrier in the trap and releasingtherefrom and digital values of logic “1” and “0”, to thereby impart tothe semiconductor field-effect transistor element a function orcapability for storing data or information even at a room temperature.

[0016] Thus, according to a first aspect of the present invention in itsmost general sense thereof, there is provided a semiconductor elementwhich includes a source region constituting a source of thesemiconductor element, a drain region constituting a drain of thesemiconductor element, an effective channel region provided between thesource region and the drain region for interconnection thereof, a gateelectrode connected to the channel region through a gate insulation filminterposed between the gate electrode and the channel region, and alevel node formed between the source region and the drain region in thevicinity of a current path in the channel region for capturing at leastone carrier, wherein effective capacitance (which will be elucidatedlater on) between the gate electrode and the effective channel region isset so small as to satisfy a condition given by the following inequalityexpression:

1/C _(gc) >kT/q ²

[0017] where C_(gc) represents the effective capacitance, k representsBoltzmann's constant, T represents an operating temperature in degreeKelvin, and q represents charge of an electron (refer to FIGS. 1A-1D).

[0018] According to another aspect of the present invention, there isprovided a semiconductor element which includes a source region and adrain region is connected to the source region through a channel regioninterposed therebetween, a gate electrode connected to the channelregion through a gate insulation film interposed between the gateelectrode and the channel region, at least one carrier confinementregion formed in the vicinity of the channel region for confining acarrier, and a potential barrier existing between the carrierconfinement region and the channel region, wherein effective capacitancebetween the gate electrode and the effective channel region is set sosmall as to satisfy a condition given by the following inequalityexpression:

1/C _(gc) >kT/q ²

[0019] where C_(gc) represents the effective capacitance, k representsBoltzmann's constant, T represents an operating temperature in degreeKelvin, and q represents charge of an electron (refer to FIGS. 10A,10B).

[0020] According to yet another aspect of the present invention, thereis provided a semiconductor element which includes a source regionconstituting a source of the semiconductor element, a drain regionconstituting a drain of the semiconductor element, the source regionbeing connected to the drain region through a channel region interposedtherebetween, a gate electrode connected to the channel region through agate insulation film interposed between the gate electrode and thechannel region, at least one carrier confinement region formed in thevicinity of the channel region for confining a carrier, and a potentialbarrier existing between the carrier confinement region and the channelregion, wherein a value of capacitance between the channel region andthe carrier confinement region is set greater than capacitance betweenthe gate electrode and the carrier confinement region, and wherein totalcapacitance existing around the carrier confinement region is so set asto satisfy a condition given by the following inequality expression:

q ²/2C _(tt) >kT

[0021] where C_(tt) represents the total capacitance, k representsBoltzmann's constant, T represents an operating temperature in degreeKelvin, and q represents charge of an electron (refer to FIGS. 10A,10B).

[0022] At this juncture, it is important to note that with the phrase“total capacitance (C_(tt)) means a total sum of capacitances existingbetween the carrier confinement region and all the other electrodes thanthe gate electrode.

[0023] In order to increase the number of times the semiconductor memoryelement can be rewritten, it is required to suppress to a possibleminimum degradation of a barrier (insulation film) existing between thechannel region and the carrier confinement region.

[0024] In view of the above, there is provided according to a furtheraspect of the invention a semiconductor element which includes a sourceregion constituting a source of the semiconductor element, a drainregion constituting a drain of the semiconductor element, the sourceregion being connected to the drain region through a channel regioninterposed therebetween, a gate electrode connected to the channelregion through a gate insulation film interposed between the gateelectrode and the channel region, at least one carrier confinementregion formed in the vicinity of the channel region for confining acarrier, the confinement region being surrounded by a potential barrier,storage of information being effectuated by holding a carrier in thecarrier confinement region, and a thin film structure having a thicknessnot greater than 9 nm and formed of a semiconductor material in aninsulation film intervening between the channel region and the carrierconfinement region (refer to FIGS. 17A, 17B).

[0025] For better understanding of the present invention, the underlyingprinciple or concept thereof will have to be elucidated in some detail.

[0026] In a typical mode for carrying out the invention, apolycrystalline silicon element (see e.g. FIGS. 1A-1D) is imparted withsuch characteristic that when potential difference between the gate andthe source thereof is increased and decreased repetitively within apredetermined range with a drain-source voltage being held constant,conductance between the source and the drain exhibits a hysteresis evenat a room temperature (see FIG. 2).

[0027] More specifically, referring to FIG. 2 of the accompanyingdrawings, when the gate-source voltage is swept vertically between afirst voltage V_(g0) (0 volt) and a second voltage V_(g1) (50 volts),the drain current of the polycrystalline silicon element exhibitshysteresis characteristic. This phenomenon has not heretofore been knownat all but discovered experimentally first by the inventors of thepresent application. The reason why such hysteresis characteristic canmake appearance will be explained below.

[0028]FIG. 4A shows a band profile in a channel region of asemiconductor device shown in FIGS. 1A-1D in the state where thegate-source voltage V_(gs) is zero volt. A drain current flows in thedirection perpendicular to the plane of the drawing. For convenience ofdiscussion, it is assumed in the following description that thedrain-source voltage is sufficiently low when compared with the gatevoltage, being however understood that the observation mentioned belowapplies equally valid even in the case where the drain-source voltage ishigh.

[0029] Now referring to FIG. 4A, there is formed in a channel (3) ofpolycrystalline silicon a potential well of low energy between a gateoxide film (5) and a peripheral SiO₂-protection film (10). In this case,energy level (11) of a conduction band in the channel region (3) whichmay be of p-type or of i-type (intrinsic semiconductor type) or n-typewith a low impurity concentration is sufficiently high when comparedwith energy level of a conduction band in a n-type source region of ahigh impurity concentration or Fermi level (12) in a degenerate n-typesource region of a high impurity concentration. As a consequence, thereexist no electrons within the channel (3). Thus, no drain current canflow.

[0030] Further, a trap level (7) exists in the vicinity of the channel(3), which can capture or trap carriers such as electrons. As levelswhich partake in forming the trap level, there are conceivable a levelextending to a grain or a level of group of grains (crystal grains inthe channel regions of polycrystalline silicon) themselves which aresurrounded by a high barrier, level internally of the grain, level at aSi—SiO₂ interface (i.e., interface between the channel region (3) andthe gate oxide film (5)), level inside the gate oxide film (5) andothers. However, it is of no concern which of these levels forms thetrap level. Parenthetically, even after the experiments conducted by theinverters, it can not be ascertained at present by which of theaforementioned levels the carriers or electrons are trapped inactuality. Of the levels mentioned above, energy in the trap level (7)which plays a role in realizing the hysteresis characteristic mentionedabove is sufficiently higher than the Fermi level (12) in the sourceregion (1). Accordingly, no electrons exist in the trap level (7). Atthis juncture, it should be added that although the trap level is shownin FIGS. 4A-4C as existing within the gate oxide film, the trap levelneed not exist internally of the oxide film. It is only necessary thatthe trap level exists in the vicinity of the channel.

[0031] As the potential difference V_(gs) between the gate (4) and thesource (1) is increased from zero volt to the low threshold voltageV_(l), potential in the channel region (3) increases. Consequently, ascompared with the initial energy level of the channel region (3) in thestate where the potential difference V_(gs) is zero (refer to FIG. 4A),the potential of the channel region (3) for electrons becomes lowerunder the condition that the potential difference V_(gs) is higher thanzero volt and lower than the low threshold voltage V_(l). When thegate-source potential difference V_(gs) has attained the low thresholdvoltage V_(l), the Fermi level in the source region (1) approaches tothe energy level in the conduction band of the channel region (3) (witha difference of about kT, where k represents Boltzmann's constant and Trepresents operating temperature in Kelvin). Consequently, electrons areintroduced into the channel region (3) from the source. Thus, a currentflow takes place between the drain and the source.

[0032] When the gate voltage is further increased, the number ofelectrons within the channel region (3) increases correspondingly.However, when the potential difference V_(gs) has reached a capturevoltage V_(g1), energy of the trap level (7) approaches to the Fermilevel (12), whereby at least one electron is entrapped or captured bythe trap level (7) because of distribution of electrons under theinfluence of thermal energy of those electrons which are introduced fromthe source region (1). At that time, since the level of the trap (7) issufficiently lower than potentials of the gate oxide (5) and peripheralSiO₂-protection film (10), the electron captured by the trap level (7)is inhibited from migration to the gate oxide film (5) and theperipheral SiO₂-protection film due to thermal energy of electron.Besides, because a grain boundary of high energy of the polycrystallinesilicon channel region (3) exists in the vicinity of the trap level (7),for example, at the Si—SiO₂ interface, the electron captured by the traplevel (7) can not move from the trap level (refer to FIG. 4C). However,since the other electrons can move, the drain current continues to flow.

[0033] In this way, once a single electron is entrapped or captured bythe trap level (7), the threshold voltage of the polycrystalline siliconsemiconductor element shown in FIGS. 1A-1D changes from the lowthreshold voltage V_(l) to the high threshold voltage V_(h), the reasonfor which will be explained below.

[0034] When the gate-source potential difference V_(gs) is lowered fromthe state shown in FIG. 4C within the range of V_(h)<V_(gs)<V_(g1), thenumber of electrons within the channel region (3) is decreased. However,in general, a high energy region exists in the periphery of the traplevel (7). Accordingly, the electron captured by the trap level (7)remains as it is (refer to FIG. 5A).

[0035] When the gate voltage is further lowered to a value at which thepotential difference V_(gs) attains the high threshold voltage V_(h),the Fermi level (12) of the source region (1) becomes different from theenergy level of the conduction band of the channel (3) by ca. kT, as aresult of which substantially all of the electrons within the channeldisappear (see FIG. 5B). Consequently, the drain current can flow nomore. However, the threshold voltage V_(h) at which no drain currentflow becomes higher than the low threshold voltage V_(l) by a voltagecorresponding to the charge of electron captured in the trap level (7).

[0036] Further, by lowering the gate-source potential difference V_(gs)to a value where the potential difference V_(gs) becomes equal to zero,potential in the peripheral high-energy region of the trap level (7)becomes lower in accompanying the lowering of the gate voltage, whichresults in that the electron captured by the trap level (7) is releasedto the region of low energy through tunneling under the effect of theelectric field (refer to FIG. 5C).

[0037] Subsequently, the gate-source potential difference V_(gs) isagain increased for the vertical sweeping. By repeating this operation,hysteresis can be observed in the drain current-versus-gate voltagecharacteristic owing to trapping and release of the electron.

[0038] In this conjunction, the inventors have discovered that thehysteresis characteristic mentioned above appears only when thecapacitance between the gate and the channel is small. Incidentally, theexperiment conducted by the inventors shows that although asemiconductor element having a gate length and a gate width each of 0.1micron can exhibit the aforementioned hysteresis characteristic, asemiconductor element whose gate length and gate width are on the orderof 1 (one) micron is incapable of exhibiting such hysteresischaracteristic.

[0039] Thus, it must be emphasized that smallness of the capacitanceC_(gc) between the gate electrode and the channel region isindispensable for the aforementioned hysteresis characteristic to makeappearance, the reason for which may be explained as follows. Thereexists between an amount of charge Q_(s) stored in the trap level and achange ΔV_(t) (=V_(h)−V_(l)) in the threshold value or voltage thefollowing relation:

ΔV _(t) =Q _(s) /C _(gc)  (1)

[0040] where C_(gc) represents capacitance between the gate and aneffective channel. With the phrase “effective channel”, it is intendedto mean a region of the channel which restrictively regulates magnitudeof a current flowing therethrough and which corresponds to a region ofhighest potential energy in the current path. Thus, this region may alsobe termed a bottle-neck region. In order to make use of theaforementioned hysteresis characteristic as the memory function, it isnecessary that the state in which the threshold value is high (V_(h))and the state where the threshold value is low (V_(l)) can definitelyand discriminatively be detected as a change in the drain current. Inother words, difference between the threshold values V_(h) and V_(l) hasto be clearly or definitely sensed in terms of a difference or changeappearing in the drain current. The conditions to this end can bedetermined in the manner described below. In general, the drain currentId of a MOS transistor having a threshold value V_(t) can be representedin the vicinity of the threshold value by the following expression:

I_(d) =A·exp[q(V _(gs) −V _(t))/(kT)]  (2)

[0041] where A represents a proportional constant, q represents chargeof an electron, V_(gs) represents a gate-source voltage of the MOStransistor, V_(t) represents the threshold voltage, k representsBoltzmann's constant and T represents an operating temperature in degreeKelvin. Thus, when V_(t)=V_(h), the drain current is given by

I _(dh) =A·exp[q(V _(gs) −V _(h))/(kT)]  (3)

[0042] while when V_(t)=V_(l), the drain current is given by

I_(dl) =A·exp[q(V _(gs) −V _(l))/(kT)]  (4)

[0043] Thus, ratio between the drain currents in the state whereV_(t)=V_(h) and the state V_(t)=V_(l) can be determined as follows:

I _(dl) /I _(dh) =exp[q(V _(h) −V _(l))/(kT)]  (5)

[0044] Thus, it can be appreciated that in order to make it possible todiscriminate the two states mentioned above from each other on the basisof the drain currents as sensed, it is necessary that the drain currentratio I_(dl)/I_(dh) as given by the expression (5) is not smaller thanthe base e (2.7) of natural logarithm at minimum, and for the practicalpurpose, the current ratio of concern should preferably be greater than“10” (ten) inclusive. On the condition that the drain current ratio isnot smaller than the base e of natural logarithm, the followingexpression holds true.

ΔV _(t)(=V _(h) −V _(l))>kT/q  (6)

[0045] Thus, from the expression (1), the following condition has to besatisfied.

Q _(s) /C _(gc) >kT/q  (7)

[0046] In order that the capture of a single electron can meet thecurrent sense condition mentioned above, it is then required that thefollowing condition be satisfied.

q/C _(gc) >kT/q  (8)

[0047] From the above expression (8), it is apparent that in order toenable operation at a room temperature, the gate-channel capacitanceC_(gc) should not exceed 6 aF (where a is an abbreviation of “atto-”meaning 10⁻¹⁸). Incidentally, in the case of the semiconductor elementhaving the gate length on the order of 1 micron, the gate-channelcapacitance C_(gc) will amount to about 1 fF (where f is an abbreviationof “femto-” meaning 10⁻¹⁵) and deviate considerably from theabove-mentioned condition. By contrast, in the case of a semiconductorelement fabricated by incarnating the teaching of the invention, thegate-channel capacitance C_(gc) is as extremely small as on the order of0.01 aF, and it has thus been ascertained that a shift in the thresholdvalue which can be sensed is brought about by the capture of only asingle even electron at a room temperature.

[0048] Further, in the course of the experiment, the inventors havefound that by holding the gate-source potential difference V_(gs)between zero volt and the voltage level V_(g1), the immediatelypreceding threshold value can be held stably over one hour or more. FIG.3 of the accompanying drawing shows the result of this experiment. Morespecifically, FIG. 3 illustrates changes in the drain current asmeasured under the condition indicated by a in FIG. 2 while holding thegate voltage to be constant. As can be seen in the figure, in the stateof low threshold value, a high current level can be held, while in thestate of high threshold value, a low current level can be held. Thus, bymaking use of the shift of the threshold value, it is possible to holdinformation or data, i.e., to store information or data, to say inanother way. Further, by sensing the drain current in these states, itis possible to read out the data. Namely, the state in which the draincurrent is smaller than a reference value 13 may be read out as logic“1” data, while the state in which the drain current is greater than thereference value (13) may be read out as logic “0” (refer to FIG. 3).

[0049] On the other hand, data write operation can be effectuated bycontrolling the gate voltage. Now, description will be directed to thedata write operation. It is assumed that in the initial state, the gatevoltage is at the low level V_(g0). By sweeping the gate voltage in thepositive direction to the level V_(g1) the threshold voltage at is setthe high level V_(h). With this operation, logic “1” of digital data canbe written in the semiconductor element according to the invention.Subsequently, the gate voltage is swept in the negative direction to thezero volt level to thereby change the threshold voltage to the low levelV_(l). In this way, logic “0” of digital data can be written.

[0050] As will now be understood from the foregoing description, it ispossible to write, hold and read the data or information only with asingle semiconductor element. This means that a memory device can beimplemented with a significantly smaller number of semiconductorelements per unit area when compared with the conventional memorydevice.

[0051] The semiconductor element according to the invention in whichdata storage is realized by capturing or entrapping only a few electronsin a storage node (which may also be referred to as the carrierconfinement region or level node or carrier trap or carrier confinementtrap, quantum confinement region or the like terms) can enjoy anadvantage that no restriction is imposed on the number of times the datacan be rewritten due to deterioration of the insulation film asencountered in a floating-gate MOSFET or restriction, if imposed, isrelatively gentle.

[0052] It is however noted that in the case of the mode illustrated inFIGS. 1A-1D for carrying out the invention, relative positionalrelationship (i.e., relative distance) between the carrier trap levelserving for the carrier confinement and the effective channel regionserving as the current path is rather difficult to fix, involvingnon-ignorable dispersions of the threshold value change characteristicamong the elements as fabricated.

[0053] As one of the measures for coping with the difficulty mentionedabove, there is proposed another mode for carrying out the inventionsuch as one illustrated in FIGS. 10A and 10B of the accompanyingdrawings in which the carrier confinement region (24) surrounded by apotential barrier is provided independently in the vicinity of a channelregion (21). With this structure, the dispersion mentioned above can bereduced.

[0054] From the stand point of performance stability of thesemiconductor element, it is preferred that dispersion of the voltagedifference ΔV_(t) between the high threshold voltage V_(h) and the lowthreshold voltage V_(l) among the semiconductor elements as fabricatedshould be suppressed to a possible minimum.

[0055] Certainly, the condition given by the expression (1) can applyvalid when the capacitance C_(gt) between the gate region and thecarrier confinement region as well as the capacitance C between thecarrier confinement region and the channel region is sufficiently small.In the other cases than the above, the condition given by the followingexpression applies valid:

ΔV _(t) =q/(1+C _(gt) /C)C _(gc)  (9)

[0056] where C_(gc) represents capacitance between the gate region (22)and the channel region (21), C_(gt) represents capacitance between thecarrier confinement region (24) and the channel (21).

[0057] In conjunction with the mode shown in FIGS. 1A-1D for carryingout the invention, the inventors have found that the term C representingthe capacitance between the carrier confinement region and the channelregion in the expression (9) is most susceptible to the dispersionbecause the carrier confinement region is so implemented as to assumethe carrier trap level. In order that the potential difference ΔV_(t)mentioned above scarcely undergoes variation notwithstanding ofvariation in the capacitance C between the carrier confinement regionand the channel region, the capacitance C_(gt) between the gateelectrode and the channel region must be sufficiently smaller than thecapacitance C (i.e., C_(gt)<C).

[0058] Thus, according to another preferred mode for carrying out theinvention, it is proposed to set at a small value the capacitance C_(gt)between the gate electrode (22) and the carrier confinement region (24)by interposing a gate insulation film (23) of a great thickness whilesetting at a large value the capacitance C between the carrierconfinement region (24) and the channel region (21) by interposingtherebetween an insulation film (25) of a small thickness.

[0059] On the other hand, in conjunction with the holding of data in thecarrier confinement region (24), it is necessary to ensure stabilityagainst thermal fluctuations. At this juncture, let's represent byC_(tt) the total capacitance existing between the carrier confinementregion and all the other regions. In general, in the absolutetemperature (T) system, energy fluctuation on the order of kT (where krepresents Boltzmann's constant and T represents temperature in degreeKelvin) will be unavoidable. Accordingly, in order to hold the datastably, it is required that change of energy given by q²/2C_(tt) asbrought about by capturing a single electron is greater than thefluctuation mentioned above. To say in another way, the condition givenby the following expression will have to be satisfied.

q ²/2C _(tt) >kT  (10)

[0060] This condition requires that the total capacitance C_(tt) definedabove has to be smaller than 3 aF inclusive in order to permit operationat a room temperature.

[0061] In still another mode for carrying out the invention asillustrated in FIGS. 17A and 17B of the accompanying drawings, a thinsemiconductor film structure (48) is formed interiorly of an insulationfilm (49, 50) which is interposed between the storage region (47) andthe channel region (46) with a view to reducing deterioration of theinsulation film (49, 50).

[0062] Thus, in the semiconductor element implemented in accordance withthe instant mode for carrying out the invention, a potential barrierprovided by the thin film structure (48) is formed interiorly of theinsulation film (49, 50) so that the thin film structure (48) playseffectively a same role as the insulation film, while making it possibleto decrease the thickness of the insulation film in practicalapplications.

[0063] As can be seen in FIGS. 17A and 17B, the semiconductor thin film(48) provided internally of the insulation film (49, 50) has an energylevel shifted by the conduction band under the effect of the quantumconfinement effect in the direction thicknesswise of the semiconductorthin film and serves essentially as a potential barrier between thestorage region and a carrier supply region for the write/eraseoperations, the reason of which will be elucidated below.

[0064] Representing the film thickness of the semiconductor thin film byL, effective mass of the carrier in the thin film by n and Planck'sconstant by h, energy in the lowest energy state in quantum fluctuationof the carrier due to the confinement effect in the thicknesswisedirection can appropriately be given by the following expression:

h²/8 mL²  (11)

[0065] In order that the energy shift due to the quantum confinementeffect is made effective in consideration of the thermal energyfluctuation, the condition given by the following inequality expression(12) is required to be satisfied.

h ²/8 mL ² >kT  (12)

[0066] In the light of the above expression (12), the thickness of thesemiconductor thin film (48) formed of silicon (Si) will have to besmaller than 9 nm inclusive in order that the barrier is effective at aroom temperature.

[0067] Thus, although there is a probability of the carrier existing inthe semiconductor thin film for a short time upon moving of the carriersbetween the channel region (46) and the carrier confinement region (47)via the insulation film (49, 50), the probability of the carriersstaying in the semiconductor thin film (48) for a long time is extremelylow. As a result of this, the semiconductor thin film (48) operates as atemporary passage for the carriers upon migration thereof between thechannel region (46) and the carrier confinement region (47), which meansthat the semiconductor thin film (48) will eventually serve as thepotential barrier because of incapability of the carrier confiningoperation.

[0068] With the structure described above, the semiconductor element canexhibit the barrier effect with the insulation film of a smallerthickness when compared with the semiconductor element in which theabove structure is not adopted. Thus, film fatigue of the insulationfilm (49, 50) can be suppressed. For further mitigating the filmfatigue, the semiconductor thin film (48) may be formed in a multi-layerstructure.

[0069] The structure in which the semiconductor thin film is provided inthe insulation film can enjoy a further advantage that the height of thepotential barrier between the carrier confinement region and the sourceregion can properly be set. Since the energy shift due to the quantumconfinement is determined in accordance with the size L of the carrierconfinement region, it is possible to adjust the height of the barrierby adjusting the film thickness in addition to the selection of the thinfilm material. In this connection, it should be noted that in thesemiconductor element of the structure known heretofore, the height ofthe barrier is determined only on the basis of the material constitutingthe insulation film.

[0070] The above other objects, features and attendant advantages of thepresent invention will more clearly be understood by reading thefollowing description of the preferred embodiments thereof taken, onlyby way of example, in conjunction with the drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

[0071]FIGS. 1A to 1D are views for illustrating a structure of a memoryelement according to a first embodiment of the invention, wherein

[0072]FIG. 1A is a top plan view,

[0073]FIG. 1B is microphotographic view of a channel portion of the same

[0074]FIG. 1C is a schematic perspective view illustrating an overallstructure of the memory element, and

[0075]FIG. 1D is a sectional view of the same taken along a line C-C′ inFIG. 1C;

[0076]FIG. 2 is a view showing graphically measured values representinga gate-source voltage dependency of a drain current of the memoryelement according to the first embodiment of the invention;

[0077]FIG. 3 is a view showing experimentally obtained results forillustrating holding of data by the semiconductor element according tothe first embodiment after writing of logic “1” and “0”;

[0078]FIGS. 4A to 4C are views for illustrating changes of a bandprofile in the vicinity of a channel region of the semiconductor elementaccording to the first embodiment of the invention when gate voltage isincreased;

[0079]FIGS. 5A to 5C are views for illustrating changes of a bandprofile in the vicinity of a channel region of the semiconductor elementaccording to the first embodiment of the invention when gate voltage islowered;

[0080]FIG. 6 is a schematic circuit diagram showing a structure of amemory IC device according to the invention in which the memory elementseach having the structure shown in FIG. 1 are employed;

[0081]FIG. 7 shows a hysteresis characteristic expected to be exhibitedby the memory device shown in FIG. 6;

[0082]FIG. 8 is an exploded perspective view showing schematically astructure of a semiconductor memory device according to the firstembodiment of the invention in which a memory cell array is formed asstacked on peripheral circuits formed in a Si-substrate surface;

[0083]FIGS. 9A and 9B are sectional views for illustrating fabricationsteps of a semiconductor memory device according to the first embodimentof the invention;

[0084]FIGS. 10A and 10B are sectional views showing a structure of asemiconductor memory element according to a second embodiment of theinvention;

[0085]FIGS. 11A and 11B are enlarged views showing exaggeratedly achannel region, a carrier confinement region and a gate electrode of thememory element according to the second embodiment of the invention,wherein

[0086]FIG. 11A is a perspective view and

[0087]FIG. 11B is a sectional view;

[0088]FIG. 12 is a view for illustrating graphically a gate-sourcevoltage dependency of a drain current in the semiconductor memoryelement according to the second embodiment of the invention;

[0089]FIGS. 13A to 13C are schematic diagrams for illustratingexaggeratedly changes in potential distribution in the vicinity of achannel region and carrier confinement region of a semiconductor memoryelement when a gate voltage is increased;

[0090]FIGS. 14A to 14C are schematic diagrams for illustratingexaggeratedly changes in potential distribution in the vicinity of achannel region and carrier confinement region of a semiconductor memoryelement when a gate voltage is lowered;

[0091]FIGS. 15A and 15B are sectional views showing a structure of asemiconductor memory element according to a third embodiment of theinvention;

[0092]FIGS. 16A to 16C are views showing a structure of a semiconductormemory element according to a fourth embodiment of the invention,wherein

[0093]FIG. 16A is a sectional view,

[0094]FIG. 16B shows a section taken along a line a-a′ in FIG. 16A and

[0095]FIG. 16C is a top plan view;

[0096]FIGS. 17A and 17B are views for illustrating a semiconductormemory element according to a fifth embodiment of the present inventionwherein

[0097]FIG. 17A is a sectional view of the same and

[0098]FIG. 17B shows a potential distribution profile in the memoryelement;

[0099]FIG. 18 is a view showing a symbol representing a semiconductormemory element according to the invention;

[0100]FIGS. 18A, 18B and 18C are views for illustrating a memory cellaccording to a sixth embodiment of the invention, wherein

[0101]FIG. 18A shows a circuit configuration of the memory cell,

[0102]FIG. 18B shows voltages applied to a word wire and a data wire ofthe memory cell upon read and write operations, respectively, and

[0103]FIG. 18C is a view for graphically illustrating dependency of adrain current on a gate-source voltage of a semiconductor elementemployed in the memory cell;

[0104]FIG. 19 is a circuit diagram showing circuit configuration of aread circuit for the memory cell according to the sixth embodiment ofthe invention;

[0105]FIG. 20 is a signal waveform diagram for illustrating timings atwhich various signals are applied upon read operation;

[0106]FIGS. 21A and 21B are diagrams showing a circuit configuration ofa 4-bit memory cell array according to the sixth embodiment and a layoutthereof, respectively;

[0107]FIGS. 22A to 22C are views showing a memory cell set according toa seventh embodiment of the invention, wherein

[0108]FIG. 22A shows a circuit configuration of the cell set,

[0109]FIG. 22B shows voltages applied to a memory element thereof uponwrite and read operations, and

[0110]FIG. 22C graphically illustrates characteristic of the memoryelement;

[0111]FIG. 23 is a circuit diagram showing a structure of asemiconductor memory device according to the seventh embodiment of theinvention;

[0112]FIGS. 24A to 24E are circuit diagrams showing variousconfigurations of the memory cell according to the invention;

[0113]FIGS. 25A to 25C are views for illustrating a memory cellaccording to an eighth embodiment of the invention, wherein

[0114]FIG. 25A shows a circuit configuration of the memory cell,

[0115]FIG. 25B shows voltages applied to a word wire and a data wire ofthe memory cell upon read and write operations, respectively, and

[0116]FIG. 25C is a view for graphically illustrating dependency of adrain current on a gate-source voltage of a semiconductor elementemployed in the memory cell;

[0117]FIG. 26 is a circuit diagram showing circuit configuration of aread circuit for the memory cell according to the eighth embodiment ofthe invention;

[0118]FIGS. 27A and 27B are circuit diagrams showing versions of thememory cell circuit according to the eighth embodiment, respectively;

[0119]FIGS. 28A and 28B are a circuit diagram showing a configuration ofa four-bit memory cell and a corresponding mask layout of the same,respectively;

[0120]FIGS. 29A to 29C are views for illustrating a memory cellaccording to a ninth embodiment of the invention, wherein

[0121]FIG. 29A shows a circuit configuration of the memory cell,

[0122]FIG. 29B shows voltages applied to a word wire and a data wire ofthe memory cell upon read and write operations, respectively, and

[0123]FIG. 29C is a view for graphically illustrating dependency of adrain current on a gate-source voltage of a semiconductor elementemployed in the memory cell;

[0124]FIG. 30 is a circuit diagram showing a read/write circuitaccording to the ninth embodiment of the invention;

[0125]FIGS. 31A, 31B and 31C are views for illustrating a memory cellaccording to a tenth embodiment of the invention, wherein

[0126]FIG. 31A shows a circuit configuration of the memory cell,

[0127]FIG. 31B shows voltages applied to a word wire and a data wire ofthe memory cell upon read and write operations, respectively, and

[0128]FIG. 31C is a view for graphically illustrating dependency of adrain current on a gate-source voltage of a semiconductor elementemployed in the memory cell;

[0129]FIG. 32 is a circuit diagram showing a read circuit according tothe tenth embodiment of the invention;

[0130]FIG. 33 is a view showing a version of a memory cell according tothe tenth embodiment; and

[0131]FIG. 34 is a block diagram showing a structure of a dataprocessing apparatus in which a memory device according to the inventionbe employed as a main memory.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0132] Now, the present invention will be described in detail inconjunction with the preferred or exemplary embodiments thereof byreference to the drawings.

[0133] Embodiment 1

[0134] Description which follows is directed to a field effectsemiconductor memory element (FET memory element) according to anexemplary embodiment of the present invention. FIGS. 1A to 1D are viewsfor illustrating a structure of a semiconductor memory element accordingto a first embodiment of the invention, wherein FIG. 1C is a schematicperspective view illustrating an overall structure of the memoryelement, FIG. 1D is a sectional view of the same taken along the lineC-C′ in FIG. 1C, FIG. 1B is an enlarged microphotographic view showing achannel portion of the same, and FIG. 1A is a top plan view thereof.Referring to the figures, a source 1 and a drain 2 are each constitutedby a region formed of n-type polycrystalline silicon and having a highimpurity concentration while a channel portion 3 is constituted by aregion formed of a non-doped polycrystalline silicon region. Each of thesource 1, the drain 2 and the channel 3 is realized in the form of athin and fine wire of polycrystalline silicon. In the case of a memorydevice manufactured actually by the inventors of the presentapplication, the channel 3 is 0.1 μm in width and 10 nm, preferably 3.4nm in thickness. Connected to the ends of the source 1 and the drain 2are contacts 1A and 2A of polycrystalline silicon, respectively, each ofwhich has a thickness greater than that of the source 1 and the drain 2,wherein the source 1 and the drain 2 are connected to metallic wiringconductors via the polycrystalline silicon contacts 1A and 2A,respectively. In the case of a typical example of the memory element,each of the polycrystalline silicon contacts 1A and 2A should preferablybe implemented with a thickness of 0.1 μm which is ten times as large asthat of the channel 3, because, if otherwise, polycrystalline siliconitself becomes insusceptible to etching upon forming contact holesdirectly in thin polycrystalline silicon. A gate electrode 4 is providedin such orientation as to intersect the channel region 3 through aninterposed gate insulation film 5. In the case of the instantembodiment, the film thickness of the gate electrode 4 is 0.1 μm. Thestructure mentioned above can best be seen from FIG. 1C.

[0135] Parenthetically, the polycrystalline silicon film constitutingthe channel region 3 is wholly enclosed by a SiO₂-protection film 10 inthe case of the instant embodiment (see FIG. 1D). Because the dielectricconstant of silicon oxide (SiO₂) is about one third of that of silicon,capacitances of the channel region 3 and the gate electrode 4 can bereduced by enclosing them with the SiO₂-protection film 10 as mentionedabove. This is one of the reasons why the hysteresis characteristicelucidated hereinbefore can be realized at a room temperature.

[0136] In the case of the memory element according to the instantembodiment, the channel of polycrystalline silicon is formed bydepositing amorphous silicon (a-Si) in a thickness of 10 nm on aSiO₂-substrate and crystallizing by heat treatment at a temperature of750° C. In this conjunction, it has been found that the thickness ofamorphous silicon (a-Si) should preferably be in the order of 3.5 nm. Astructure of a channel portion is shown in FIG. 1B. In the course of theheat treatment, silicon crystal grains in amorphous silicon growprogressively. However, when the size of the grain reaches the filmthickness, any further growth in the direction perpendicular to theplane of the film is prevented. At the same time, the rate of the graingrowth in the direction parallel to the film becomes retarded. As aconsequence, the grain size in the lateral direction (i.e., in thedirection parallel to the film surface) is substantially equal to thefilm thickness. For these reasons, the field-effect semiconductor memoryelement according to the instant embodiment of the invention featuresthat the grain size of polycrystalline silicon forming the channelregion is extremely small.

[0137] The small grain size mentioned above contributes to realizationof small capacitance between the gate electrode and the channel region,the reason for which will be elucidated below. In the field effectelement now under consideration, it is only a few current paths 6 havinglowest resistance in the channel region 3 that a current can actuallyflow within a low-current range close to a threshold level (see FIG.1A). To say in more concrete, the current flow takes place due tomigration or transfer of electrons from one to another crystals grain.In the case of the instant embodiment, the current path is extremelyfine or thin because of a very small grain size as mentioned above.Consequently, the region in which electrons exists is remarkably smallwhen compared with whole the channel region. For this reason, thecapacitance C_(gc) which is effective between the gate electrode and theeffective channel portion (in the sense defined hereinbefore) issignificantly small.

[0138] In the case of a semiconductor memory element actually fabricatedaccording to the instant embodiment, the gate-channel capacitance C_(gc)mentioned above was set at an extremely small value, e.g. 0.02 aF(atto-Farad), with a view to observing the effect of change in thethreshold value to a possible maximum extent. As a result of this, therange of voltages required for operation expanded to several ten volts.Of course, by setting the gate-channel capacitance C_(gc) at a greatervalue, e.g. 0.2 aF, the operation voltage range can be set to a range ofseveral volts usually employed in the conventional integrated circuit.To this end, the thickness of the gate insulation film 5 may bedecreased and/or the length or width of the gate electrode may beincreased, which can be realized without any appreciable technicaldifficulty.

[0139] In the case of the instant embodiment of the invention, thechannel is formed of polycrystalline silicon. At this juncture, itshould however be mentioned that the hysteresis characteristic can berealized even in a conventional bulk MOSFET formed in a crystal siliconsubstrate if the gate-channel capacitance mentioned above can be made sosmall that the conditions mentioned previously can be satisfied. In thatcase, the bulk MOSFET can be made use of as a memory element. In thisconjunction, it is however noted that in the case of a bulk MOSFET, theeffects of the grain mentioned above are absent. Besides, the lower sideof the bulk MOSFET is covered with a Si-film having a high dielectricconstant. Consequently, it is necessary to decrease the size of the bulkMOSFET element when compared with the element having the channel formedof polycrystalline silicon. This in turn means that difficulty will beaggravated in manufacturing the bulk MOSFET memory element. However,because the bulk MOSFET has a greater mobility of carriers, it canhandle a large current and is suited for a high-speed operation, to anadvantage. As a further version, the hysteresis characteristic mentionedpreviously can be realized by using a MOSFET of SOI(Silicon-On-Insulator) structure as well. The SOI structure can beimplemented by growing monocrystalline silicon on an insulation film andby forming a MOSFET therein. Because the gate-channel capacitance of theSOI MOSFET can be made smaller than that of the bulk MOSFET, thehysteresis characteristic can be realized with a greater size whencompared With the bulk MOSFET.

[0140] The foregoing description has been made on the assumption thatthe channel for migration of electrons is of n-type. It should howeverbe mentioned that similar operation can be accomplished by using holes.Further, other semiconductor material than silicon can be employed informing the channel region.

[0141] Additionally, it has been assumed in the foregoing descriptionthat the gate electrode 4 is located beneath the channel region 3.However, similar operation can be effectuated equally with suchstructure in which the gate electrode lies above the channel region.Besides, gate electrodes may be provided above and beneath the channel,respectively, for realizing similar operation and effects as thosementioned previously. Furthermore, the gate electrode may be disposed ata side laterally of the channel region. Moreover, gate electrodes may beprovided at both sides of the channel, respectively.

[0142] Now, referring to FIG. 6, description will be made of anintegrated memory circuit which is comprised of the semiconductorelements of the structure described above. FIG. 6 shows a structure of amemory IC device in which polycrystalline silicon memory elements eachhaving the structure shown in FIG. 1 are employed. In this conjunction,it is assumed that each of the semiconductor elements or thepolycrystalline silicon memory elements has such hysteresischaracteristic as illustrated in FIG. 7. More specifically, it ispresumed that when a voltage V_(w) is applied between the gate and thesource, the memory element takes on logic “1” state (state of highthreshold value represented by V_(h)) while upon application of avoltage of −V_(w) between the gate and the source, the memory elementassumes logic “0” state (low threshold state V_(l)). On the other hand,application of a voltage in a range of −V_(w)/2 to V_(w)/2 between thegate and the source or between the gate and the drain, the thresholdvoltage undergoes no change. The characteristic illustrated in FIG. 7 iscomparable to that shown in FIG. 2 except that the threshold value islowered as a whole and can be realized by introducing a donor impurityin the channel region of the memory element upon manufacturing thereof.

[0143] Referring to FIG. 6, each of semiconductor memory elements MP1 toMP4 is constituted by a semiconductor element according to the inventionwhich has the structure shown in FIG. 1 and the hysteresischaracteristic illustrated in FIG. 7. Each of the semiconductor memoryelements has a gate terminal connected to a word wire, a drain terminalconnected to a data wire and a source terminal connected to the groundpotential.

[0144] Operation for writing digital data in the integrated memorycircuit is performed through cooperation of a word wire driver circuitand a data wire driver circuit shown in FIG. 6 in a manner describedbelow. For writing logic “1” in the memory element MP1, the potential onthe word wire 1 is set to a voltage level of V_(w)/2 with the potentialof the data wire 1 being set to −V_(w)/2, while the other word wires anddata wires are set to zero volt. As a result of this, a voltage of V_(w)is applied between the gate and the drain of the memory element MP1,which thus takes on the logic “1” state (high threshold state). At thistime point, all the other memory elements than the memory element MP1are applied with a voltage not higher than V_(w)/2. Accordingly, nochange takes place in the threshold voltage in these other memoryelements. On the other hand, for writing logic “0” in the memory elementMP1, the potential on the word wire 1 is set to −V_(w)/2 with thepotential on the data wire 1 being set to V_(w)/2. Thus, the voltage of−V_(w) is applied between the gate and the drain of the memory elementMP1, whereby the memory element MP1 is set to logic “0” state (lowthreshold state V_(l)). At this time point, all the other memoryelements than the memory element MP1 are applied with a voltage which isnot higher than −V_(w)/2. Accordingly, no change can take place in thethreshold value in these other memory elements.

[0145] On the other hand, reading of information or data is carried outin a manner described below (see FIG. 6). In the data wire drivercircuit, the data wire is connected to a voltage source via a loadelement. On the other hand, the other end of the data wire is connectedto a sense amplifier. Now, operations involved in reading out data fromthe memory element MP1 will be considered. To this end, the potential ofthe word wire 1 as selected is set to the level of zero volt while thepotential on the other word wire 2 not selected is set to the voltagelevel of −V_(w)/2. When the memory element MP1 is in the logic “1”state, this means that the memory element MP1 is in the off-state (i.e.,non-conducting state) with the data wire remaining in the logically highstate. Even when the memory element MP2 is in the logical “0” state, nocurrent can flow through the memory element MP1 because the word wirenot select is at the potential level of −V_(w)/2. When the memoryelement MP1 is in the logic “0” state, a current flows from the datawire 1 to the grounded wire via the memory element MP1, resulting inlowering of the potential at the data wire 1. This potential drop isamplified by the sense amplifier, whereupon the data read-out operationcomes to an end. The memory device can be implemented in this manner.

[0146] In the memory device now under consideration, peripheral circuitsthereof such as a decoder, the sense amplifier, an output circuit andthe like are implemented by using the conventional bulk MOSFET formed ina surface of a Si-substrate in such an arrangement as illustrated inFIG. 8, and a memory cell array including the memory elements MP1 to MP4each of the structure illustrated in FIG. 1 are fabricated on theperipheral circuits with an interposition of an insulation film. This isbecause polycrystalline silicon for the memory elements MP1 to MP4 canbe fabricated on the bulk MOSFETs. By virtue of this structure, thespace or area otherwise required for the peripheral circuits can bespared, whereby the memory device can be implemented with about twice ashigh an integration density when compared with that of the conventionaldynamic RAM. Parenthetically, it should be added that a wiring layerwhich exists in actuality between the bulk MOSFETs and thepolycrystalline silicon transistor layer is omitted from illustration inFIG. 8.

[0147] As will be appreciated from the foregoing description, with thestructure of the memory device according to the instant embodiment ofthe invention, there can be realized a integrated memory circuit with ahigh integration density because of capability of storing single-bitinformation by the single memory element. Besides, the integrationdensity can further be increased by stacking the memory cell array onthe peripheral circuit layer in a laminated or stacked structure.Additionally, there is no necessity for reading out a quantity ofelectric charge, as required in the case of the conventional dynamicRAM, but the signal can be generated on the data wire in a staticmanner, so to say. Owing to this feature, fine structurization canfurther be enhanced without involving degradation in the signal-to-noiseratio (S/N ratio). Moreover, information as stored can be retained overan extended time period, which means that refreshing operation asrequired in the case of the dynamic RAM can be rendered unnecessary.Consequently, power consumption can be suppressed to a possible minimum.Further, the peripheral circuits can be implemented in much simplifiedconfiguration. Owing to the features mentioned above, there can berealized according to the teachings of the invention incarnated in theinstant embodiment a semiconductor memory device with an integrationdensity which is at least twice as high as that of the conventionaldynamic RAM while the cost per bit can be reduced at least to a half ofthat required in the conventional dynamic RAM. Of course, electric powerrequired for holding or retention of information (data) cansignificantly be reduced.

[0148] In the foregoing description, it has been assumed that the lowthreshold voltage V_(l) is of negative polarity with the high thresholdlevel V_(h) being positive, as illustrated in FIG. 7. However, even whenthese threshold voltages V_(l) and V_(h) for the memory element are setat higher levels, respectively, similar operation can be ensured simplyby setting correspondingly higher the gate control signal level.

[0149] Next, by reference to FIGS. 9A and 9B, description will turn to aprocess for fabricating or manufacturing the memory element and thememory device according to the instant embodiment of the invention. Atfirst, an n-channel MOS 15 and a p-channel MOS 16 (i.e., a CMOS(Complementary Metal-Oxide Semiconductor device) are fabricated on asurface of a p-type Si-substrate 14, which is then followed by formationof an insulation film over the CMOS device as well as formation of metalwires 17 (refer to FIG. 9A). Subsequently, an inter-layer insulationfilm 18 is deposited and the surface thereof is flattened for reducingroughness. Next, a polycrystalline silicon region which is to serve as agate electrode 4 of the memory element is formed on the flat surface ofthe insulation layer 18. To this end, the polycrystalline silicon regionis doped with n-type impurity at a high concentration so that itexhibits a low resistance. Next, a SiO₂-film which is to serve as a gateinsulation film 5 is deposited in thickness on the order of 50 nm overthe insulation layer 18 having the gate electrodes through a chemicalvapor deposition method (i.e., CVD method in abbreviation), which isthen followed by deposition of an amorphous silicon layer. Afterpatterning of the amorphous silicon layer, source regions 1 and drainregions 2 are doped with n-type impurity such as As, P or the likethrough ion implantation and annealed at a temperature of about 750° C.,whereby channels 3 of polycrystalline silicon are formed. Finally, aprotection or passivation film 10 of SiO₂ is formed. Thus, there can befabricated a memory device of high integration density according to theinvention (refer to FIG. 9B). At this juncture, it should be added thatan electrically conducting layer may be provided on the top surface ofthe memory device for the purpose of shielding the memory device againstnoise to thereby enhance the reliability thereof.

[0150] Embodiment 2

[0151]FIGS. 10A and 10B are sectional views showing a memory elementaccording to a second embodiment of the invention. An SOI(Silicon-On-Insulator)-substrate is employed as the substrate, whereinFIG. 10B shows a section taken along as line a-a′ in FIG. 10A. A sourceregion 19 and a drain region 20 are each constituted by an n-typesilicon region of high impurity concentration and low resistance,wherein a channel 21 of silicon extending between the source and drainregions 19 and 20 is formed in a fine or thin wire. A thin film 25 ofSiO₂ is formed over the channel 21. Further, a storage node 24 forconfining carriers with silicon grains is formed on the channel region21. A gate electrode 22 is provided above the channel region 21 with agate insulation film 23 being interposed therebetween.

[0152] With the structure of the memory element according to the instantembodiment, the capacitance C_(gc) between the channel region 21 and thegate electrode 22 can be reduced because of a very small wire width ofthe channel 21. Writing and erasing operations can be effected bychanging potential level. More specifically, the writing can be carriedout by injecting electrons from the channel region into the storage node24 by clearing a potential barrier provided by the insulation film 25,while for erasing the stored information, electrons are drawn out fromthe storage node 24. Thus, in the memory element according to theinstant embodiment, writing and erasure of or data information to andfrom the storage node 24 are performed by transferring the electronswith the channel. It should however be mentioned that these operationscan be realized through electron transferring with other region than thechannel region. The same holds true in the embodiments of the inventionwhich will be described below. Further, although silicon is employed forforming the source, the drain and the channel with SiO₂ being used forforming the insulation films in the memory element according to theinstant embodiment, it should be understood that the source and thedrain may be formed of other semiconductor material or metal and thatthe insulation film may also be formed with other compositions so longas the capacitance C_(gc) satisfying the requisite conditions mentionedpreviously can be realized.

[0153] Additionally, it is important to note that although the storagenode 24 is provided above the channel 21 in the memory element accordingto the instant embodiment, the storage node 24 may be provided beneaththe channel region or at a location laterally of the channel region.Besides, although it has been described that the SOI substrate isemployed with monocrystalline silicon being used for forming the source,the drain and the channel, it should be understood that they may beformed by using polycrystalline silicon as in the case of the firstembodiment. In that case, difference from the first embodiment can beseen in that the storage node 24 is provided independently. It shouldfurther be added that the material for the insulation film interposedbetween the channel region and the storage node need not be same as thematerial of the insulation film interposed between the gate and thestorage node.

[0154] Although it is presumed that the carriers are electrons in thememory element and the memory device according to the instantembodiment, holes may equally be employed as the carriers substantiallyto the same effect. This holds true in the embodiments described belowas well.

[0155] According to the teachings of the invention incarnated in theinstant embodiment, the storage node 24 is formed by using crystalgrains of a small size, wherein the storage node 24 of Si-grains issurrounded or enclosed by the gate insulation film 23 and the insulationfilm 25 of SiO₂ to thereby reduce surrounding parasitic capacitance.Because of the small size of the grains constituting the storage node24, the surrounding or total capacitance C_(tt) therefor may bedetermined in terms of intrinsic capacitance. In the case of a sphericalbody having a radius r and enclosed by a material having a dielectricconstant ε, the intrinsic capacitance thereof is given by 4πεr. By wayof example, for the storage node formed by silicon crystal grains havinga grain size of 10 nm, the surrounding or total capacitance C_(tt) ofthe storage node is about 1 aF.

[0156]FIGS. 11A and 11B show schematically and exaggeratedly a channelregion, a carrier confinement node and a gate electrode in a perspectiveview and a sectional view, respectively.

[0157] Referring to FIG. 12, when a gate-source voltage (i.e., voltageapplied between the gate and the source) is swept between a firstvoltage V_(g0) (zero volt) and a second voltage V_(g1) (5 volts) in thevertical direction as viewed in FIG. 12, the drain current exhibits ahysteresis characteristic. In this conjunction, relevant potentialdistributions on and along a plane b-b′ in FIG. 11B are illustrated inFIGS. 13A to 13C and FIGS. 14A to 14C. The reason why the hysteresischaracteristic such as illustrated in FIG. 12 makes appearance will beelucidated below.

[0158] In the semiconductor memory element shown in FIG. 10, potentialdistribution making appearance in the channel region 21 when thepotential difference V_(gs) between the gate and the source is zero voltis schematically shown in FIG. 13A. This corresponds to the state 25shown in FIG. 12. Parenthetically, it is assumed that the drain currentflows in the direction perpendicular to the plane of the drawing FIG.13A. The description which follows will be made on the assumption thatthe drain-source voltage is sufficiently low as compared with the gatevoltage, being however understood that the following description appliesvalid as it is, even when the voltage between the drain and the sourceis high.

[0159] Now referring to FIG. 13A, in the channel region 21 surrounded bya potential barrier 25 formed between the channel region 21 and thestorage node 24 and the peripheral SiO₂-film 23, there prevails alow-energy potential. Thus, the storage node 24 (carrier confinementregion) formed of Si-grains and surrounded by the insulation films 23and 25 can capture or trap the carriers or electrons. On the other hand,no electrons exist in the channel region 21 because energy level of theconduction band in the channel region 21 of P-type or N-type having lowimpurity concentration or i-type (intrinsic semiconductor type) issufficiently higher than the energy level of the conduction band in theN-type source 19 of a high impurity concentration or Fermi level in theN-type degenerate source region 19 having a high impurity concentration.Consequently, no drain current can flow.

[0160] Incidentally, energy in the carrier confinement region or thestorage node 24 is sufficiently higher than the Fermi level in thesource region 19. Thus, no electron exists in this region 24 either.

[0161] As the potential difference V_(gs) between the gate electrode 22and the source 19 is increased from zero volt to the low thresholdvoltage V_(l), potential in the channel region 21 increases. As aconsequence, potential in the channel region 21 for electrons becomeslower, as can be seen in FIG. 13B, hereby electrons are introduced intothe channel region 21 from the source 19. Thus, a current flow takesplace between the source and the drain.

[0162] When the gate voltage is further increased, the number ofelectrons existing in the channel region 21 increases correspondingly.However, when the gate-source voltage V_(gs) reaches a writing voltageV_(g1), energy in the storage node 24 becomes low, being accompaniedwith a corresponding increase of the potential gradient between thechannel 21 and the storage node 24. As a consequence of this, at leastone electron will be entrapped in the storage node 24 by clearing thepotential barrier 25 due to thermal energy distribution of electronand/or tunneling phenomenon (tunnel effect). This corresponds totransition from the state 27 to the state 28, as illustrated in FIG. 12.

[0163] Thus, there takes place a Coulomb blockade owing to one electrontrapped in the storage node 24 as well as potential increase, wherebyinjection of another electron in the storage node 24 is prevented, as isillustrated in FIG. 14A.

[0164] In this way, every time one electron is entrapped in the storagenode 24, the threshold voltage of the semiconductor memory element shownin FIG. 10 changes from the low threshold V_(l) to the high thresholdvoltage V_(hs), the reason for which will be explained below.

[0165] When the gate-source voltage V_(gs) is lowered within the rangeof V_(h) (high threshold voltage) <V_(gs)<V_(l) (low threshold voltage),starting from the state illustrated in FIG. 14A, the number of electronsin the channel region 21 decreases. However, electron captured ortrapped in the storage node 24 remains as it is, because of existence ofthe potential barrier 25 between the storage node 24 and the channel 21.

[0166] When the voltage of the gate electrode 22 is lowered to a levelwhere the potential difference V_(gs) is equal to the high thresholdvoltage V_(h), the Fermi level in the source 19 becomes different fromthe energy level of the conduction band in the channel 21 by a magnitudeon the order of kT, as a result of which substantially all of theelectrons in the channel region make disappearance, (refer to FIG. 14B).This corresponds to the state 29 shown in FIG. 12. At this juncture, itshould however be mentioned that the threshold value V_(h) at which thedrain current can no more flow becomes higher than the low thresholdvoltage V_(l) by an amount of the charge of the electrons captured inthe storage node 24.

[0167] As the gate-source voltage V_(gs) is further lowered to a levelwhere it becomes equal to zero volt, the potential gradient between thestorage node 24 and the channel region 21 becomes steepercorrespondingly, as a result of which the electron captured in thestorage node 24 is released owing to the tunneling effect brought aboutby thermal energy distribution of electrons and the field effect (referto FIG. 14C). Potential profile in the state where electrons aredispelled is equivalent to the initial potential profile illustrated inFIG. 13A. This means that the semiconductor memory element resumes thestate 25 shown in FIG. 12.

[0168] Subsequently, when the gate-source voltage V_(gs) is againincreased for effecting repeatedly the sweep in the vertical direction,hysteresis phenomenon which accompanies the capture/release of electroncan be observed.

[0169] In the structure of the memory element now under consideration,the condition given by the expression (8) has to be satisfied in orderto detect the presence/absence of a single electron in terms of acurrent.

[0170] Next, description will turn to a method of fabricating the memoryelement or memory device according to the instant embodiment of theinvention. AS is shown in FIGS. 10A and 10B, the source region 19, thedrain region 20 and the channel region 21 are formed in the SOIsubstrate by resorting to a photoetching process. The channel region isrealized in the form of a fine or thin wire. The source and drainregions are doped with n-type impurity at a high concentration. Bycontrast, the channel region is doped with n-type or i-type or p-typeimpurity at a low impurity concentration. Subsequently, the SiO₂-film 25is deposited through a CVD (chemical vapor deposition) process, which isthen followed by formation of a crystal silicon grain or the storagenode 24 through a CVD process.

[0171] In order to form the silicon crystal grain 24 (which is to serveas the storage node 24) having a very small radius r, a nucleus formedinitially in the CVD deposition process is made use of for forming thecrystal silicon grain 24. To this end, formation of the crystal silicongrain 24 by the CVD method should be carried out at a low temperatureand completed within a short time.

[0172] Embodiment 3

[0173]FIG. 15A and 15B show in sections a memory element according to athird embodiment of the present invention, respectively, in which FIG.15B is a sectional view taken along a line a-a′ in FIG. 15A. The memoryelement or memory device according to the instant embodiment differsfrom the second embodiment in that the former is implemented in such astructure in which a channel region 33 and a carrier confinement regionor storage node 34 are sandwiched between a pair of gate electrodes 31and 32. Thus, in the memory element or memory device according to theinstant embodiment, writing and erasing operations can be performed notonly from the first gate electrode 31 but also through the medium of thesecond gate electrode 32.

[0174] In the case of memory element or memory device according to thesecond embodiment of the invention, it is expected that potentialprofiles in the carrier confinement region and in the vicinity of thechannel region inclusive thereof may undergo variation under theinfluence of change in the external potential. By contrast, the memoryelement or memory device according to the instant embodiment is lesssusceptible to the influence of such external potential change owing tothe shielding effect of the gate electrodes provided at both sides, toan additional advantage.

[0175] Embodiment 4

[0176]FIGS. 16A to 16C show a memory element according to a fourthembodiment of the invention, wherein FIG. 16A is a sectional view, FIG.16B shows a section-taken along a line a-a′ in FIG. 16A and FIG. 16C isa top plan view. Referring to the figures, formed over a channel region39 of a bulk MOSFET in which a source 35 and a drain 36 are formed in asilicon semiconductor crystal substrate is an insulation film 40 onwhich a plurality of silicon crystal grains 41 are formed. Further, aninsulation film 42 is formed over the insulation film 40 and the grains41. Additionally, a second gate electrode 38 is deposited on theinsulation film 42. This gate electrode 38 is of such a shape that a gapexists in the direction interconnecting the source 35 and the drain 36.A first gate electrode 37 is provided above the second gate electrode 38with an insulation film 43 being interposed therebetween. The source 35and the drain 36 are each constituted by a region formed of an n-typebulk silicon having a high impurity concentration, wherein a p-typeregion 44 intervenes between the source region 35 and the drain 36.

[0177] By applying a voltage of positive or plus 1 polarity to the firstgate electrode 37, electrons are induced in a surface portion of thep-type region 44, whereby a channel 39 is formed. In that case, thepotential of the second gate electrode 38 is set lower than the firstgate electrode 37 so that the second gate electrode 38 also operates asan electrostatic shield electrode. As a result of this, the channelregion 45 is formed only in a region located in opposition to the finegap of the second gate electrode 38, whereby the effective capacitanceC_(gc) between the first gate electrode 37 and the channel region 39 canbe made smaller. Writing and erasing operations can be realized bychanging the potential of the first gate electrode 37 or the second gateelectrode 38 or the substrate 37 in a substantially same manner asdescribed hereinbefore in conjunction with the third embodiment.

[0178] Embodiment 5

[0179]FIG. 17A shows a cross section of a memory element according to afifth embodiment of the present invention. The direction in which thecurrent flows extend perpendicularly to the plane of the drawing. Thechannel region and the carrier confinement region (storage node) as wellas regions located in the vicinity are shown exaggeratedly. The sourceand the drain are implemented in same configurations as those of thememory element according to the second embodiment of the invention. Theinstant embodiment differs from the second embodiment in that a thinfilm 48 of silicon is formed in SiO₂-insulation films 49 and 50 betweena channel region 46 of silicon and a storage node (carrier confinementnode) 47 formed by a silicon crystal grain.

[0180] Carriers within a channel 46 can reach the storage node (carrierconfinement region) 47 via the Si-thin film 48. FIG. 17B shows apotential profile in the memory element of the structure mentionedabove. Referring to FIG. 17B, an energy shift 52 takes place in theSi-thin film 48 due to the quantum confinement effect in the directionthicknesswise. The thin Si-film 48 plays a role as a barrier for themigration of electron from the Si-channel region 46 to the carrierconfinement region (storage node) 47. As a result of this, for achievingthe same barrier effect, the sum of film thicknesses of the SiO₂-films49 and 50 existing between the channel and the carrier confinementregion may be reduced as compared with the film thickness of theSiO₂-film located between the channel region and the carrier confinementregion of the memory element in which the structure according to theinstant embodiment is adopted (e.g. refer to FIGS. 10A and 10B).Accordingly, fatigue of the insulation film can be mitigated, wherebythe number of the times the memory is rewritten can be increased.

[0181] It should further be mentioned that the potential barrierrealized by making use of the quantum confinement effect described aboveis effective for protecting the insulation film against fatigue even inthe case where a greater number of carriers are to be handled by thecarrier confinement region.

[0182] Embodiment 6

[0183] A structure of a memory read circuit for a semiconductor memorydevice according to the invention will be described by reference toFIGS. 18A to 18C and FIG. 19. In the description which follows, thesemiconductor memory element according to the invention which may be oneof the elements described hereinbefore by reference to FIGS. 1A-1D, FIG.6, FIGS. 10A, 10B, FIGS. 15A, 15B, FIGS. 16A-16C and FIGS. 17A, 17B,respectively, is identified by representing the carrier trapping node(carrier confinement region) by a solid circle as shown in FIG. 18 forthe purpose of discrimination from the conventional field effecttransistor. On FIGS. 18A to 18C, FIG. 18A shows a circuit configurationof a single-bit memory cell, FIG. 18B shows voltages applied to a wordwire W and a data wire D upon read and write operations, respectively,and FIG. 18C graphically illustrates a dependency of a drain current ona gate voltage (gate-source voltage) in a semiconductor element MM7employed for realizing the memory cell. The circuit configuration per seis identical with that described hereinbefore in conjunction with thefirst embodiment by reference to FIG. 6.

[0184]FIG. 19 shows a circuit configuration for reading data orinformation stored in a memory cell MM1. Needless to say, a large numberof memory cells similar to the memory cell MM1 are disposed in an arrayin the memory device which the invention concerns, although illustrationthereof is omitted. The memory cell MM1 serving for storing informationdiffers from the conventional MOSFET known heretofore in that the valueof a current which can be handled by the memory cell is smaller ascompared with that of the MOSFET. This is because the gate-channelcapacitance is set small in the case of the memory cell according to theinvention. A structure for reading such a small current value stably ata high speed will be described below. The memory cell constituted by thesemiconductor memory element MM1 is connected to a data wire D which inturn is connected to an input transistor M9 constituting a part of adifferential amplifier via a data wire selecting switch M5. Connected toanother data wire Dn provided in pair with the data wire D are dummycells constituted by semiconductor memory elements MM5 and MM6,respectively. The data wire Dn is connected to a gate terminal of aninput transistor constituting the other part of the differentialamplifier via a data wire selecting switch M6 .

[0185] Now, description will be directed to operation for reading datafrom the memory cell MM1. FIG. 20 shows timing of signals involved inthe read operation. It is assumed that logic. “0” is written in thememory cell MM1 which is thus in the state where the threshold voltageis low. Each of the dummy cells MM5 and MM6 is always written with logic“0” previously. Upon read operation, a signal S2 is set to a low levelto thereby precharge both the data wires D and Dn to a source voltageV_(r). At the same time, signals S3 and S4 are set to a high level tothereby allow the data wires D and Dn to be connected to the inputtransistors M9 and M10 of the differential amplifier, respectively.Further, at the same timing, signals S5 and S6 are set to the high levelto thereby activate the differential amplifier so that the outputs OUTand OUT_(n) are equalized to each other. By changing potentials of theword wire WI and WD from the low level to the high level, the memorycell MM1 and the dummy cells MM5 and MM6 are selected. Then, the memorycell MM1 assumes the on-state (conducting state), which results in thatthe potential of the data wire D becomes low. At the same time, thedummy cells MM5 and MM6 are set to the on-state, whereby the potentialof the data wire Dn becomes low. However, because the dummy cells MM5and MM6 are connected in series, the current driving capability thereofis poor as compared with that of the memory cell MM1. Consequently, thepotential of the data wire Dn changes more gently than that of the datawire D. When data of the data wires D and Dn are fixed, a signal S6 isset to the low level, whereby the differential amplifier can assume thestate ready for operation. The potential difference between the datawires D and Dn is amplified by the differential amplifier, the outputOUT of which thus assumes the high level while the other output OUT_(n)becomes low. At this time point, operation for reading logic “0” fromthe memory cell MM1 is completed.

[0186] When the memory cell MM1 is in the state of logic “1” (i.e., inthe state where the threshold value is high with only a small currentflowing), the data wire D remains in the precharged state, as a resultof which the potential of the data wire Dn lowers more speedily thanthat of the data wire D. The resultant difference is then amplified bythe differential amplifier, whereupon the read operation comes to anend.

[0187] For reading information from the memory cell constituted by asemiconductor memory element MM2, the semiconductor memory elements MM3and MM4 then serve as the dummy cells. It is sufficient to provide asingle dummy cell for each of the data wires. Thus, the area requirementcan be suppressed to a minimum.

[0188] With the circuit arrangement described above, information readoperation can be effectuated even when only a small potential differencemakes appearance between the data wires D and Dn. This means that thequantity of charge to be discharged from the data wire D via the memorycell MM1 may be small. By virtue of these features, high-speed operationcan be realized.

[0189] In the case of the exemplary embodiment described above, theseries connection of the dummy cells MM5 and MM6 is provided as themeans for making the dummy cell current substantially equal to a half ofthe memory cell current. However, the reference potential can begenerated by reducing the channel width to a half or lowering theapplied gate voltage instead of resorting to the provision of the serialdummy-cell connection.

[0190]FIGS. 21A and 21B show a circuit configuration of memory cells ina semiconductor memory device and a layout thereof, respectively. Morespecifically, FIG. 21A is a circuit diagram showing four memory cellsarrayed adjacent to one another, while FIG. 21B shows a mask layoutcorresponding to the circuit configuration shown in FIG. 21A. The twomemory cells MM91 and MM92 connected to a word wire W91 share one andthe same gate electrode in common, whereby the wiring required, ifotherwise, can correspondingly be spared. On the other hand, for theother memory cells MM93 and MM91 which are connected to a same data wireD91, diffused layers thereof are directly connected to each other forallowing a single contact (CT) to be shared by both the memory cellsMM93 and MM91, whereby the wiring area as required is correspondinglyreduced.

[0191] Embodiment 7

[0192] Another embodiment of the semiconductor memory device accordingto the invention will be described by reference to FIGS. 22A to 22C andFIG. 23. With the structure of this embodiment, the read operation canbe carried out at a higher speed than the semiconductor memory deviceaccording to the sixth embodiment.

[0193] Of these drawings, FIG. 22A shows a circuit diagram of a cell setcomprised of an assembly of plural memory cells MM51, MM52 and MM53which are connected to the same sub-data wire D, FIG. 22B shows voltagesapplied to the memory element MM51 upon write and read operations, FIG.22C graphically illustrates characteristic of the memory element MM51,and FIG. 23 shows a structure of a semiconductor memory deviceimplemented by using the cell sets each of a structure shown in FIG.22A. The instant embodiment differs from the sixth embodiment primarilyin that the data wire is hierachized into a main data wire MD 51 and asub-data wire D (see FIG. 23) in order to carry out read operation at ahigher speed. As can be seen in FIG. 22A, the source terminals of thememory cells MM51, MM52 and MM53 are connected to the sub-data wire D,which in turn is connected to a preamplifier comprised of transistorsM53 and M52 and generally denoted by PA51. The preamplifier PA51 has anoutput terminal connected to a main data wire MD 51 (see FIG. 23).Connected to the main data wire MD 51 are a plurality of cell sets eachof the structure mentioned above via the respective preamplifiers. Themain data wire MD 51 is connected to one of the input terminals of amain amplifier MA51 constituted by a differential amplifier. A column ofdummy cells is constituted by cell sets disposed in an array. The dummycell (e.g. MM54) is connected to another main data wire MD 52 via apreamplifier PA52. The main data wire MD 52 in turn is connected to theother input terminal of the main amplifier MA51. The preamplifier PA52for the dummy cell set is so designed that the current drivingcapability thereof approximately corresponds to a half of that of thepreamplifier PA51. This can be realized, for example, by diminishing thechannel width of the transistor to the half.

[0194] Next, description will turn to operation for reading informationfrom a memory cell MM51. Information of logic “0” is written in thedummy cell MM54 previously. It is first assumed that information oflogic “0” is stored in the memory cell MM51. At first, high-levelpotential V_(r) is applied to a gate terminal S52 of the transistor M51to thereby set the source terminal S51 to the ground potential level,whereby the sub-data wire D is set to the ground potential level.Further, for the selection of cell set, high-level potential is appliedto the gate terminal S53 to thereby set the transistor M52 of thepreamplifier PA51 to the conducting state (on-state). At the same time,the main data wires MD 51 and the MD 52 are precharged to the highpotential level V_(r). When the potential of the word wire W changesfrom a low level to a high level V_(r), the memory cell MM51 becomesconductive, whereby the sub-data wire D is charged from a sourceterminal P (=V_(r)) via the memory cell MM51. Consequently, thetransistor M53 is turned on, which results in that the main data wire MD51 is discharged through the memory cells MM52 and MM53 with thepotential of the main data wire MD 51 being lowered. Through similaroperation, the dummy cell MM54 connected to the same word wire assumesthe on-state. In response, the preamplifier PA52 operates to cause themain data wire MD 52 to be discharged. Thus, the potential of the maindata wire MD 52 is lowered. However, because the current drivingcapability of the preamplifier PA52 is poor as compared with that of thepreamplifier PA51, the potential of the main data wire MD 52 is loweredat a slower rate than that of the main data wire MD 51. Thus, theremakes appearance between the main data wires MD 51 and MD 52 a potentialdifference, which is detected by the main amplifier MA51, wherebycorresponding output information is derived from the main amplifierMA51. Operation for reading out logic “1” is carried out in the similarmanner.

[0195] In the case of the instant embodiment, it is sufficient for thememory cell MM51 only to drive the sub-data wire D. The sub-data wirefeatures that the parasitic capacitance is small, because the number ofthe cells connected to the sub-data wire is as small as in a range of 8to 32 and because the length of the sub-data wire is short. Thus, thesub-data wire can be driven by the memory cell or memory element MM51 ata high speed. Equally, high-speed operation of the main data wire MD 51can be achieved because it can be driven at a high speed by thepreamplifier PA51.

[0196] According to the teaching of the invention incarnated in theinstant embodiment, the preamplifiers PA52 and PA51 are so implementedthat they differ in respect to the current driving capability for thepurpose of generating a reference voltage for the differential amplifierPA51. When compared with the sixth embodiment in which the current isreduced to a half by the memory cell per se, the instant embodimentaccording to which the current level is changed in the preamplifierconstituted by the transistors of higher rating is advantages in that itis less susceptible to the influence of the dispersions mentionedhereinbefore.

[0197] Parenthetically, the main amplifier MA51 can be implemented byusing an appropriate one of various circuits known in the art such asdifferential amplifier employed in the device of the sixth embodiment, acurrent-mirror type differential amplifier circuit and the like.

[0198] In the case of the sixth and seventh embodiments described above,it has been assumed that the memory cell is constituted by a singletransistor. It should however be mentioned at this juncture that thememory cell may be implemented in other configurations such asexemplified by those shown in FIGS. 24A to 24E. More specifically, FIG.24A shows a memory cell in which a back gate is provided in oppositionto the gate electrode with the channel being interposed between the backgate and the gate electrode. This structure of the memory cell providesan advantage that when a plurality of memory cells are connected to asame back gate terminal, information or data contained in these memorycells can simultaneously be set to logic “0” by applying a voltage ofminus polarity to the back gate. Of course, by applying a voltage ofplus or positive polarity to the back gate, it is equally possible towrite simultaneously logic “1” in these memory cells.

[0199] In this junction, the back gate terminal may be realized bymaking use of the semiconductor substrate itself, a potential well orthe like.

[0200]FIG. 24B shows a memory cell in which the terminal wire P extendsin parallel with the word wire so that control of the memory device canbe performed on a row-by-row basis independently. On the other hand,FIG. 24C shows a memory cell in which the terminal wire P extends inparallel with the data wire. Further, FIG. 24D shows a memory cell inwhich the gate of the memory element MM73 is connected to the data wire.In this case, the terminal P can be spared, which contributes toreduction of the area as involved in implementing the semiconductormemory device. Finally, FIGS. 24E shows a memory cell in which the gateof the memory element MM74 is connected to the word wire and which thuscan ensure an advantage similar to that of the memory cell shown in FIG.24D.

[0201] Embodiment 8

[0202]FIGS. 25A to 25C and FIG. 26 show a semiconductor memory deviceaccording to an eighth embodiment of the invention. As can be seen inFIG. 25A, the memory cell of the memory device according to the instantembodiment is constituted by a circuit including a memory element MM21according to the invention and a switching FET (field-effect transistor)M25 which are connected in series. More specifically, the word wire isconnected to the gate of the switching FET M25 so that the voltageapplied to the memory element MM21 from the data wire D can beinterrupted by the switching FET M25. Thus, necessity for applying avoltage to non-selected memory cells which shares the word wire or thedata wire with the selected memory cell can be obviated. This in turnmeans that the device according to the instant embodiment is excellentover the sixth and seventh embodiments in respect to the data holdcharacteristic, to an advantage.

[0203] Writing operation for the memory cell according to the instantembodiment is performed in a manner described below. First, operationinvolved in writing logic “0” will be considered. Applied to the wordwire to be selected is a voltage of (V_(cc)+V_(t)) while the potentiallevel of zero volt is applied to the data wire to be selected. As aresult, the switching FET M25 is turned on, whereby a node N21 assumesapproximately the ground potential level. Since the source terminal P isat a voltage level of V_(cc)/2, a voltage of −V_(cc)/2 is applied acrossthe gate and the source of the memory element MM21, whereby informationof logic “0” is written in the memory cell (refer to FIG. 25C). Next,operation for writing logic “1” is considered. Also in this case, thevoltage of (V_(cc)+V_(t)) is applied to the word wire while applying thevoltage V_(cc) to the data wire. Thus, the voltage V_(cc)/2 is appliedbetween the gate and the source of the memory element MM21, wherebylogic “1” is written in the memory cell (refer to FIG. 25C).

[0204] The operation for reading data or information from the memorycell according to the instant embodiment can be carried out by the meansof the similar to those adopted in the sixth and seventh embodiments.However, in connection with the instant embodiment, the inventionteaches an arrangement which allows the read/write operation to beperformed at a lower source voltage. Referring to FIG. 26, for readingout information from the memory cell comprised of the memory element M25and the switching FET MM21, the potential level of the word wire W21 ischanged to the source voltage level V_(cc) from the ground potentiallevel, and at the same time the potential of the word wire WD22 of thedummy cell comprised of a switching FET M27 and memory elements MM25 andMM26 is changed from low level to high level. Succeeding operation isthe same as that of the sixth embodiment except that after the output isfixed, rewriting is performed for the memory cell by a writing driverconnected to the output of the sense amplifier. By way of example, whenlogic “1” is to be written in the memory element MM21, the voltageV_(cc) is applied to the data wire D. In that case, a voltagesubstantially equal to V_(cc) is applied across the gate and the sourceof the memory element MM21, whereby logic “1” can be written in thememory element MM21. On the other hand, when logic “0” is to be written,the data wire is set to the ground potential level. Thus, the voltage of−V_(cc)/2 is applied between the gate and the source of the memoryelement MM21, whereby logic “0” is written in the memory cell.

[0205] In the memory device according to the instant embodiment, everytime the data read operation is performed, rewriting operation iscarried out in succession. By virtue of this arrangement, inversion ofthe information or data held by the memory element MM21 from logic “0”to logic “1” will present no problem so long as such inversion takesplace only after the potential difference of such a magnitude whichenables the read operation has occurred between the data wire D and thedummy data wire Dn. Thus, the read voltage V_(r) and the write voltageV_(cc)/2 can be set at values or levels which are relatively close toeach other. This in turn means that the write voltage can be set at alow level. By way of concrete example, the read voltage V_(r) may be setat 3 volts with the write voltage V_(cc)/2 being set at 4 volts. Bycontrast, in order to ensure positively prevention of the information ordata inversion from occurrence in the read operation as describedhereinbefore in conjunction with the seventh embodiment (see FIG. 22C),the write voltage V_(p) has to be set at about three times as high asthe read voltage V_(r). This necessitates application of a high voltagefor the write operation.

[0206]FIGS. 27A and 27B are circuit diagrams showing versions of thememory cell circuit according to the instant embodiment, respectively.The memory cell shown in FIG. 27A differs from the one shown in FIG. 25Ain that a source terminal P is connected to the gate of the memoryelement MM81. On the other hand, in the memory cell shown in FIG. 27B,the gate of the memory element MM82 is controlled by a control signal Csupplied externally of the memory cell.

[0207]FIGS. 28A and 28B show a circuit configuration and a layout of asemiconductor memory device including a number of memory cells each ofthe structure shown in FIG. 27A which corresponds to four bits. In thesefigures, the memory cells MM101 to 104 are each constituted by thepolycrystalline silicon memory element described hereinbefore inconjunction with the first embodiment. As can be seen from FIG. 28B, theword wires for the adjacent memory cells are constituted by one and thesame electrode, while a contact is shared in common by the two adjacentmemory cells and connected to the data wire. It will thus be understoodthat the area required for implementation of the memory cell cansignificantly be decreased.

[0208] Embodiment 9

[0209]FIGS. 29A to 29C show a memory cell circuit and a read circuitaccording to a ninth embodiment of the invention. More specifically,FIG. 29A shows a circuit diagram of a memory cell according to theinstant embodiment, FIG. 29B shows voltages as applied upon read andwrite operations performed for the memory cell, and FIG. 29C graphicallyillustrates characteristics of memory elements MM31 and MM32 employed inthe memory cell. A feature of the memory cell according to the instantembodiment of the invention resides in that complementary information ordata are written in the memory elements MM31 and MM32. Morespecifically, for writing logic “1”, a voltage of V_(cc) is applied tothe word wire W while a voltage of V_(e) (of negative polarity) isapplied to the data wire D, as a result of which a switching FET M33 isturned on, whereby the potential of the data wire D is applied to a nodeN31 which thus assumes the potential level V_(e). Since the voltageV_(e) is applied between the gate and the source of the memory elementMM32, the latter is set to a low threshold state. In contrast, a voltageof (V_(cc)−V_(e)) is applied between the gate and the source of thememory element MM31, which thus assumes a high threshold state. Forwriting logic “0” in the memory cell, the data wire D is set to thewrite voltage level V_(p). As a result of this, the memory element MM31assumes the low threshold state with the memory element MM32 in the highthreshold state. In succession to the write operation, the potentiallevel of the data wire is set to V_(w)/2, which results in applicationof voltage of about V_(cc)/2 between the gates and the sources of thememory elements MM31 and MM32, respectively. In the logic “1” state, thedata wire D tends to discharge, while in the state of logic “O”, thedata wire D is charged. This trend or state is detected by thedifferential amplifier for reading the data or information, as can beseen in FIG. 30.

[0210] In the memory cell according to the instant embodiment of theinvention, the potential level of the data wire lowers or rises independence on whether the information or data of the memory cell to beread out is logic “1” or “0”. Accordingly, it is possible to applydirectly the reference voltage (V_(cc)/2) to one of input terminals ofthe differential amplifier. For this reason, no dummy cell is required,to an advantage. In this conjunction, it should be recalled that in thecase of the circuit configurations according to the embodimentsdescribed hereinbefore, the dummy cells have to be provided because itis indefinite whether the potential level of the data wire is maintainedor lowered in dependence on whether the memory cell data is logic “1” or“0”.

[0211] Embodiment 10

[0212] Description will now turn to a memory cell circuit according to afurther embodiment of the invention by reference to FIGS. 31A to 31C, inwhich FIG. 31A shows a memory cell circuit for a single bit according tothe instant embodiment of the invention, FIG. 31B shows voltages forread and write operations, respectively, and FIG. 31C graphicallyillustrates characteristics of the memory elements MM41 and MM42. In thememory cell according to the instant embodiment, such arrangement isadopted that a pair of memory cells each of the structure shown in FIG.27A can be selected by means of one and the same word wire. To this end,memory elements MM41 and MM42 are adapted to store information or datawhich are complementary to each other. Namely, when the memory elementMM41 is set to a low threshold state, the memory element MM42 is set toa high threshold state, and vice versa. Consequently, when the word wireis set to a high potential level after the write operation, there makesappearance between the data wires D and Dn a potential differencereflecting a difference in the current driving capability between thememory elements MM41 and MM42. Thus, by connecting the data wires D andDn to a pair of input terminals of a differential amplifier, it ispossible to read information or data stored in the memory cell.

[0213] In the memory cell or memory device according to the instantembodiment of the invention, stable operation can be ensured withoutneed for provision of the dummy cell as well as need for generation ofthe reference potential level for the differential amplifier. Thus, thecircuit design can be simplified. Parenthetically, similar advantage canbe assured by using a memory cell circuit shown in FIG. 33.

[0214] In the foregoing description of the exemplary embodiments, it hasbeen assumed that an n-channel gate insulated field effect transistor isemployed as the switching element. It goes, however, without saying thatit may be replaced by other type of switching element. By way ofexample, a p-channel field effect transistor may be employed. In thatcase, the polarity of the voltage applied to the gate electrode must ofcourse be inverted.

[0215] Besides, in the foregoing description, it has been assumed thatthe semiconductor memory element is of n-channel type. It is howeverobvious that the memory element as well as the memory device can beimplemented by using p-channel memory element (i.e., element capable ofoperating with holes).

[0216] Embodiment 11

[0217] The semiconductor memory devices or simply the memories describedhereinbefore in conjunction with the sixth to tenth embodiments featurethat information or data can be held without being volatilized. Thus,the time taken for data write operation is extremely short when comparedwith the conventional non-volatile memory, and no limitation is imposedto the number of times the rewriting operation is performed. Further,because the writing operation is completed by injecting only a fewelectrons, the writing operation of a very high speed can be achieved.The reason why no limitation is imposed on the number of times for thewriting operation can be explained by the fact that the writing isrealized by the move of a few electrons.

[0218] The memory devices according to the invention can very profitablybe employed as a main memory of a microprocessor in a data processingsystem such as shown in FIG. 34. Since the memory device according tothe instant embodiment is nonvolatile, information stored once in thememory device can be held even after a source power supply isinterrupted. Owing to this feature, the external storage implemented inthe form of a hard disk or floppy disk can be realized by a memory chipfabricated according to the teachings of the invention. Besides, becauseof nonvolatileness of the main memory, a computer incorporating thistype of main memory can instantaneously be restored to the stateprevailing immediately before interruption of the power supply.

[0219] Additionally, by using the semiconductor memory device describedin conjunction with the sixth to tenth embodiments as a cache memory ina microprocessor, not only the cache memory can be made nonvolatile butalso power consumption of the microprocessor can be decreasedsignificantly.

[0220] As is apparent from the foregoing description, there is providedaccording to the invention the semiconductor memory devices which can beimplemented with a small number of memory elements which per se haveinformation or data storing capability while mitigating the requirementimposed on the area for implementation without need for cooling at acryogenic level of temperature. Thus, by using the semiconductor memorydevice according to the invention, there can be realized a nonvolatilememory device susceptible to high speed rewrite operation.

We claim:
 1. A semiconductor memory comprising: a field effecttransistor having a source, a drain and a gate; a carrier confinementregion formed of a conductor or a semiconductor; a data line; and a wordline; said word line controlling a gate potential of said field effecttransistor; and said carrier confinement region being connected to saiddata line through a source-drain path of the field effect transistor,wherein said gate potential in an information read operation is set tobe positive relative to a source potential of said field effecttransistor.
 2. A semiconductor memory according to claim 1, wherein saidgate potential is set at zero in an information hold state.
 3. Asemiconductor memory according to claim 1, wherein said gate potentialin an information write operation is set to be positive relative to asource potential of said field effect transistor, and the relativemagnitude of said gate potential to said source potential in aninformation write operation is larger than that in an information readoperation.